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Sterile Neutrino Oscillations and CP-Violation Implications for MiniBooNE NuFact’07 Okayama, Japan

Sterile Neutrino Oscillations and CP-Violation Implications for MiniBooNE NuFact’07 Okayama, Japan. Georgia Karagiorgi, Columbia University August 10, 2007. Outline. Sterile neutrino oscillation formalism Oscillation analysis Constraints from MiniBooNE result

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Sterile Neutrino Oscillations and CP-Violation Implications for MiniBooNE NuFact’07 Okayama, Japan

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  1. Sterile Neutrino Oscillations and CP-Violation Implications for MiniBooNENuFact’07Okayama, Japan Georgia Karagiorgi, Columbia University August 10, 2007

  2. Outline • Sterile neutrino oscillation formalism • Oscillation analysis • Constraints from MiniBooNE result • Preliminary oscillation analysis results • CPV Implications and Future Studies at MiniBooNE Georgia Karagiorgi, Columbia U.

  3. Sterile Neutrino Oscillation Formalism • 3 active + n sterile neutrinos: • lightsterile neutrinos • they don’t interact thru standard weak couplings • they have very small active flavor content (Ue4,Uμ4, …, Uen, Uμn) •  can participate in neutrino oscillations • For example, for 2 sterile neutrinos (3+2): Oscillation: Disappearance: νe νμ ντ νs Georgia Karagiorgi, Columbia U.

  4. Oscillation Analysis Neutrino oscillations and disappearance due to sterile neutrinos can be constrained by short-baseline experiments (sensitive to high Δm2) We are interested in: • constraining the oscillation parameters by a combined analysis of SBL data • studying the compatibility of null SBL results with LSND and MiniBooNE results in a 3 active + n sterile neutrino hypothesis constraint (90%CL) Georgia Karagiorgi, Columbia U.

  5. Oscillation Analysis Using data from short baseline experiments: • Start with unoscillated signal predictions from: • Generate model parameters (importance sampling via Markov chain) • For each set of parameters, • get signal prediction after oscillation/disappearance for all experiments considered • compare signal prediction to experimental data and calculate , goodness-of-fit for each experiment considered, and combined , goodness-of-fit • determine allowed regions by Gaussian approx. Dataset: LSND, KARMEN, NOMAD, MB, CCFR, CDHS, CHOOZ, BUGEY (+ atm constraint) # of bins: 5 9 30 8 18 15 14 60 (1) appearance experiments disappearance experiments Model acceptance probability: Georgia Karagiorgi, Columbia U.

  6. Oscillation Analysis 3+n model parameter assumptions: Approximation: m1≈ m2≈ m3≈ 0  n independent mass splittings: 2n moduli of mixing parameters: Ue4, Uμ4, … n-1 Dirac CPV phases 0.1eV2 ≤ ≤ 100eV2(motivated by LSND signal) (imposed by atm and solar data) Atmospheric constraint: upper limit: CP violation option: Fix , or allow to vary within For example, for 3+2 oscillations: 2 indep. mass splittings: 4 moduli: 1 CPV phase: No CPV allowed for 3+1 models! [M. Maltoni, et al., hep-ph/0405172] Georgia Karagiorgi, Columbia U.

  7. Constraints from MiniBooNE Recent MiniBooNE result implies that MiniBooNE is incompatible with LSND within 2-neutrino oscillation hypothesis. [see talk by C. Polly] Calls for more complicated oscillation scenario (e.g., 3+2, CPV, …) in order to reconcile the two results. Interested in “low-E excess” and implications for 3+n We consider the full energy range data (300 MeV < E < 3000 MeV) in our analysis. “A Search for Electron Neutrino Appearance at the Δm2 ~ 1eV2 Scale,” The MiniBooNE Collaboration [hep-ex/0704.1500]. Georgia Karagiorgi, Columbia U.

  8. MiniBooNE Dataset Allow both: (oscillations) and: ( disappearance) ( background disappearance) Use a ratio method: Compare: ratio from MC prediction (first principles) after applying oscillation, disappearance, disappearance to: ratio from data MC prediction = nbinsBooNE = 8, ndfBooNE = nbinsBooNE – 2nsterile –2nsterile– (nsterile-1) NEW!!! with energy spectrum (full νμνe conversion; takes into account different cross sections) intrinsic ~0.5% of beam full MiniBooNE error matrix (scaled to MC prediction) [see talk by K. Mahn] CPV case Georgia Karagiorgi, Columbia U.

  9. Preliminary Oscillation Results: 3+1 3+1 already excluded from previous studies (independent of MiniBooNE result) MiniBooNE oscillation upper limits in 3+1 scenario: [See, e.g.: M. Sorel, et al., hep-ph/0305255 and talk by T. Schwetz] 1 1 1 90% CL excluded regions Single-sided raster scan, 2 dof P r e l i m i n a r y Georgia Karagiorgi, Columbia U.

  10. Preliminary Oscillation Results: 3+1 3+1 already excluded from previous studies (independent of MiniBooNE result) MiniBooNE oscillation upper limits in 3+1 scenario: [See, e.g.: M. Sorel, et al., hep-ph/0305255 and talk by T. Schwetz] 90% CL excluded regions Single-sided raster scan, 2 dof P r e l i m i n a r y Georgia Karagiorgi, Columbia U.

  11. Preliminary Oscillation Results: 3+1 3+1 already excluded from previous studies (independent of MiniBooNE result) MiniBooNE disappearance upper limits in 3+1 scenario: [See, e.g.: M. Sorel, et al., hep-ph/0305255] 1 0 0 1 90% CL excluded regions Single-sided raster scan, 2 dof P r e l i m i n a r y Georgia Karagiorgi, Columbia U.

  12. Preliminary Oscillation Results: 3+1 3+1 already excluded from previous studies (independent of MiniBooNE result) MiniBooNE disappearance upper limits in 3+1 scenario: [See, e.g.: M. Sorel, et al., hep-ph/0305255] 0 0 1 90% CL excluded regions Single-sided raster scan, 2 dof P r e l i m i n a r y Georgia Karagiorgi, Columbia U.

  13. Preliminary Oscillation Results: 3+2 For comparison, we show 2 analyses: • MiniBooNE data with oscillations only • MiniBooNE data with oscillations andand disappearance In both cases we show results from fits with: • Appearance only experiments • All experiments combined Georgia Karagiorgi, Columbia U.

  14. Preliminary Oscillation Results: 3+2Allowing Only Oscillations in MiniBooNE Data Appearance-only experiments: KARMEN, MB, LSND, NOMAD CPC CPV P r e l i m i n a r y P r e l i m i n a r y 90%CL 99%CL Georgia Karagiorgi, Columbia U.

  15. Preliminary Oscillation Results: 3+2Allowing and Disappearance Also Appearance-only experiments: KARMEN, MB, LSND, NOMAD CPC CPV P r e l i m i n a r y P r e l i m i n a r y 90%CL 99%CL Georgia Karagiorgi, Columbia U.

  16. Preliminary Oscillation Results: 3+2Allowing Only Oscillations in MiniBooNE Data Combined analysis: all experiments CPC CPV P r e l i m i n a r y P r e l i m i n a r y 90%CL 99%CL Georgia Karagiorgi, Columbia U.

  17. Preliminary Oscillation Results: 3+2Allowing and Disappearance Also Combined analysis: all experiments CPC CPV P r e l i m i n a r y P r e l i m i n a r y 90%CL 99%CL Georgia Karagiorgi, Columbia U.

  18. General Remarks for 3+2 • There are allowed 3+2 regions • Allowing and disappearance along with oscillations to describe MiniBooNE data does not seem to either favor or disfavor combined fits, compared to only allowing • There is no preference for CPC vs. CPV scheme • Best fit models: • CPC combined analysis: • CPV combined analysis: Georgia Karagiorgi, Columbia U.

  19. CP-Violation: Implications for MiniBooNE Allowed MiniBooNE oscillation probability asymmetry within 3+2 oscillation scenario: MC predicted MiniBooNE full-osc rates 90%CL 99%CL Allowed region obtained using constraints from null SBL + LSND experiments only [G. K. et al., hep-ph/0609177]. Georgia Karagiorgi, Columbia U.

  20. CP-Violation: Implications for MiniBooNE MiniBooNE asymmetry predicted based on 3+2 best fit model for CPV combined analysis: 90%CL 99%CL Asymmetry significance ~ 1 assuming 6x1020 POTin both neutrino and antineutrino running mode (data collected as of now: neutrino mode: 7.0x1020 POT antineutrino mode: 2.4x1020 POT) Georgia Karagiorgi, Columbia U.

  21. Conclusions • Both CPC and CPV 3+2 oscillation scenarios are allowed by a combined analysis of SBL data, including LSND and MiniBooNE • MiniBooNE provides strong limits on oscillations and limits on and disappearancewithin a 3+1 hypothesis • MiniBooNE data: important in addressing the viability of sterile neutrino models • Leptonic CP-violation possibility opened up in the 3+2 sterile neutrino hypothesis could have measurable effects at MiniBooNE • A longer running in anti-neutrino mode would allow more detailed studies of CPV scenario and more confident determination of a possible CPV phase Georgia Karagiorgi, Columbia U.

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